Lecture 6 Newtons Third Law Newtons 3 rd

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Lecture 6: Newton’s Third Law • Newton’s 3 rd Law • Action-reaction pairs •

Lecture 6: Newton’s Third Law • Newton’s 3 rd Law • Action-reaction pairs • Inclined coordinate system • Massless ropes and massless, frictionless pulleys • Coupled objects

Newton’s 3 rd Law Common version: For every action there is an equal and

Newton’s 3 rd Law Common version: For every action there is an equal and opposite reaction. * *This is problematic because it suggests that first there is an action and then there is a reaction. Better version:

Action-reaction pairs

Action-reaction pairs

Example: object at rest on a table Forces of action-reaction pair act on two

Example: object at rest on a table Forces of action-reaction pair act on two different objects

Object on inclined plane Normal = perpendicular Normal force must be perpendicular to surface

Object on inclined plane Normal = perpendicular Normal force must be perpendicular to surface Weight: vertically down

Object on inclined plane Choose axis in direction of acceleration. Draw components of weight

Object on inclined plane Choose axis in direction of acceleration. Draw components of weight vector Identify θ in the weight triangle

Components of weight vector In this coordinate system:

Components of weight vector In this coordinate system:

Coupled objects: ropes and pulleys We make the following approximations: • massless, un-stretchable rope

Coupled objects: ropes and pulleys We make the following approximations: • massless, un-stretchable rope → tension is constant throughout the rope • massless, frictionless pulley → tension remains constant as rope passes over pulley Caution: If mass and spatial extension of the pulley are taken into account, the tension does not remain constant! We will study this with Rotational Motion in lectures 18 -21.

Example with coupled objects Two blocks are connected by a massless string. A block

Example with coupled objects Two blocks are connected by a massless string. A block of mass m is on a frictionless inclined plane that makes angle θ with the vertical, while a block of mass M hangs over a massless and frictionless pulley. Derive an expression for the acceleration of the blocks in terms of relevant system parameters.